Optical alignment systems and methods for wavelength beam combining laser systems

ABSTRACT

In various embodiments, wavelength beam combining laser systems incorporate fast-axis collimation lenses and slow-axis collimation lenses (either separately or as portions of a single hybrid lens) optically upstream of an optical rotation system to thereby reduce or minimize cross-talk in the combined output beam.

RELATED APPLICATIONS

This application is a continuation of U.S. patent application Ser. No.14/735,269, filed Jun. 10, 2015, which claims the benefit of andpriority to U.S. Provisional Patent Application No. 62/011,909, filedJun. 13, 2014, U.S. Provisional Patent Application No. 62/012,336, filedJun. 14, 2014, and U.S. Provisional Patent Application No. 62/028,149,filed Jul. 23, 2014, the entire disclosure of each of which is herebyincorporated herein by reference.

TECHNICAL FIELD

In various embodiments, the present invention relates to laser systems,specifically optical alignment systems for wavelength beam combininglaser systems.

BACKGROUND

High-power laser systems are utilized for a host of differentapplications, such as welding, cutting, drilling, and materialsprocessing. Such laser systems typically include a laser emitter, thelaser light from which is coupled into an optical fiber (or simply a“fiber”), and an optical system that focuses the laser light from thefiber onto the workpiece to be processed. The optical system istypically engineered to produce the highest-quality laser beam, or,equivalently, the beam with the lowest beam parameter product (BPP). TheBPP is the product of the laser beam's divergence angle (half-angle) andthe radius of the beam at its narrowest point (i.e., the beam waist, theminimum spot size). The BPP quantifies the quality of the laser beam andhow well it can be focused to a small spot, and is typically expressedin units of millimeter-milliradians (mm-mrad). A Gaussian beam has thelowest possible BPP, given by the wavelength of the laser light dividedby pi. The ratio of the BPP of an actual beam to that of an idealGaussian beam at the same wavelength is denoted M², or the “beam qualityfactor,” which is a wavelength-independent measure of beam quality, withthe “best” quality corresponding to the “lowest” beam quality factor of1.

Wavelength beam combining (WBC) is a technique for scaling the outputpower and brightness from laser diode bars, stacks of diode bars, orother lasers arranged in one- or two-dimensional array. WBC methods havebeen developed to combine beams along one or both dimensions of an arrayof emitters. Typical WBC systems include a plurality of emitters, suchas one or more diode bars, that are combined using a dispersive elementto form a multi-wavelength beam. Each emitter in the WBC systemindividually resonates, and is stabilized through wavelength-specificfeedback from a common partially reflecting output coupler that isfiltered by the dispersive element along a beam-combining dimension.Exemplary WBC systems are detailed in U.S. Pat. No. 6,192,062, filed onFeb. 4, 2000, U.S. Pat. No. 6,208,679, filed on Sep. 8, 1998, U.S. Pat.No. 8,670,180, filed on Aug. 25, 2011, and U.S. Pat. No. 8,559,107,filed on Mar. 7, 2011, the entire disclosure of each of which isincorporated by reference herein.

A variety of WBC techniques have been utilized to form high-power lasersfor a host of different applications, and such techniques often involvethe formation and manipulation of beams having fast and slow divergingaxes. One of the problems that may arise when using an optical rotationsystem (or “optical rotator,” or “beam twister,” or “optical twister”)to individually rotate each beam emitted by an array of emitters is thatthe final combined beam may have a skewed or twisted profile. This maybe caused in part when one of the axes of the beam (i.e., fast or slow)continues to diverge through the optical rotation system, which mayinclude or consist essentially of two (or two arrays of) cylindricallenses. Placement of a fast axis collimating (FAC) lens before theoptical rotation system typically sufficiently collimates the fastdiverging axis (FA) such that the beam may fully rotate through opticalrotation system. The FAC lens is generally able to sufficientlycollimate the FA due to the rapid divergence of the beam(s) along theFA. However, the slow diverging axis (SA) generally does not diverge asquickly, so lenses downstream of the optical rotation system have beenused to collimate the beam and help minimize the M² value, which isdesired for WBC systems. Furthermore, the slow divergence and size ofthe emitted beams along the SA are generally addressed via a “far field”optical solution downstream of the optical rotation system. Thus, thereis a need for optical systems and methods for WBC systems that reducedivergence along the SA via components disposed upstream of an opticalrotation system.

SUMMARY

In accordance with embodiments of the present invention, wavelength beamcombining (WBC) laser systems feature multiple emitters (or “beamemitters”), e.g., diode bars or the individual diode emitters of a diodebar, which are combined using a dispersive element to form amulti-wavelength beam. Each emitter in the system individually resonatesand is stabilized through wavelength-specific feedback from a commonpartially reflecting output coupler that is filtered by the dispersiveelement (e.g., a diffraction grating, a dispersive prism, a grism(prism/grating), a transmission grating, or an Echelle grating) alongthe beam-combining dimension. In this manner, laser systems inaccordance with embodiments of the present invention producemulti-wavelength output beams having high brightness and high power.

In accordance with various embodiments of the present invention, thelaser system features an optical arrangement (or “system”) placeddownstream from the array of beam emitters and upstream of an opticalrotation system. (Herein, “downstream” or “optically downstream,” isutilized to indicate the relative placement of a second element that alight beam strikes after encountering a first element, the first elementbeing “upstream,” or “optically upstream” of the second element.) Theoptical arrangement may include or consist essentially of, for example,a FAC lens closely followed (i.e., closely upstream of) a SAC lens. Invarious embodiments, the FAC lens and the SAC lens may even be portionsof a unitary hybrid lens that is disposed downstream of the array ofbeam emitters and upstream of the optical rotation system. The unifiedhybrid lens may be a single piece that is molded to incorporate the FACand SAC lenses, or may include or consist essentially of a FAC-lensportion optically bonded to a SAC-lens portion.

In various embodiments, the SAC lens being disposed so close to the beamemitters results in incomplete collimation of the beams along the SA.However, even this incomplete collimation helps to reduce negativecross-talk between the slow axis and fast axis that may result whenbeams pass through the optical rotation system. Such cross-talk betweenthe slow axis and fast axis may deleteriously impact (e.g., skew) theresulting combined beam and render optical coupling the combined beam(e.g., into an optical fiber) more difficult. However, this may beaddressed, at least in part, in various embodiments of the invention viareducing the focal length of (and thus the separation between) thelenses of the optical rotation system (e.g., two cylindrical lenses).The reduction in focal length and separation depends on the index ofmaterial. For example, the separation of optical rotators using fusedsilica that are available commercially may be a few millimeters inmagnitude. The typical output beam rotation in the far field may be onthe order of 20-40 degrees. By using a higher index glass the separationbetween the two lenses may be 2-3 times shorter. This reduction inseparation may result in the output beam rotation in the far field of afew degrees. This focal-length reduction may help minimize cross-talkbetween the slow axis and fast axis within the optical rotation systemand improve the profile of the combined output beam.

Embodiments of the present invention couple the one or more input laserbeams into an optical fiber. In various embodiments, the optical fiberhas multiple cladding layers surrounding a single core, multiplediscrete core regions (or “cores”) within a single cladding layer, ormultiple cores surrounded by multiple cladding layers.

Herein, “optical elements” may refer to any of lenses, mirrors, prisms,gratings, and the like, which redirect, reflect, bend, or in any othermanner optically manipulate electromagnetic radiation. Herein, beamemitters, emitters, or laser emitters, or lasers include anyelectromagnetic beam-generating device such as semiconductor elements,which generate an electromagnetic beam, but may or may not beself-resonating. These also include fiber lasers, disk lasers, non-solidstate lasers, vertical cavity surface emitting lasers (VCSELs), etc.Generally, each emitter includes a back reflective surface, at least oneoptical gain medium, and a front reflective surface. The optical gainmedium increases the gain of electromagnetic radiation that is notlimited to any particular portion of the electromagnetic spectrum, butthat may be visible, infrared, and/or ultraviolet light. An emitter mayinclude or consist essentially of multiple beam emitters such as a diodebar configured to emit multiple beams. The input beams received in theembodiments herein may be single-wavelength or multi-wavelength beamscombined using various techniques known in the art.

Laser diode arrays, bars and/or stacks, such as those described in thefollowing general description may be used in association withembodiments of the innovations described herein. Laser diodes may bepackaged individually or in groups, generally in one-dimensionalrows/arrays (diode bars) or two dimensional arrays (diode-bar stacks). Adiode array stack is generally a vertical stack of diode bars. Laserdiode bars or arrays generally achieve substantially higher power, andcost effectiveness than an equivalent single broad area diode.High-power diode bars generally contain an array of broad-area emitters,generating tens of watts with relatively poor beam quality; despite thehigher power, the brightness is often lower than that of a broad arealaser diode. High-power diode bars may be stacked to produce high-powerstacked diode bars for generation of extremely high powers of hundredsor thousands of watts. Laser diode arrays may be configured to emit abeam into free space or into a fiber. Fiber-coupled diode-laser arraysmay be conveniently used as a pumping source for fiber lasers and fiberamplifiers.

A diode-laser bar is a type of semiconductor laser containing aone-dimensional array of broad-area emitters or alternatively containingsub arrays containing, e.g., 10-20 narrow stripe emitters. A broad-areadiode bar typically contains, for example, 19-49 emitters, each havingdimensions on the order of, e.g., 1 μm×100 μm. The beam quality alongthe 1 μm dimension or fast-axis is typically diffraction-limited. Thebeam quality along the 100 μm dimension or slow-axis or array dimensionis typically many times diffraction-limited. Typically, a diode bar forcommercial applications has a laser resonator length of the order of 1to 4 mm, is about 10 mm wide and generates tens of watts of outputpower. Most diode bars operate in the wavelength region from 780 to 1070nm, with the wavelengths of 808 nm (for pumping neodymium lasers) and940 nm (for pumping Yb:YAG) being most prominent. The wavelength rangeof 915-976 nm is used for pumping erbium-doped or ytterbium-dopedhigh-power fiber lasers and amplifiers.

A diode stack is simply an arrangement of multiple diode bars that candeliver very high output power. Also called diode laser stack, multi-barmodule, or two-dimensional laser array, the most common diode stackarrangement is that of a vertical stack which is effectively atwo-dimensional array of edge emitters. Such a stack may be fabricatedby attaching diode bars to thin heat sinks and stacking these assembliesso as to obtain a periodic array of diode bars and heat sinks There arealso horizontal diode stacks, and two-dimensional stacks. For the highbeam quality, the diode bars generally should be as close to each otheras possible. On the other hand, efficient cooling requires some minimumthickness of the heat sinks mounted between the bars. This tradeoff ofdiode bar spacing results in beam quality of a diode stack in thevertical direction (and subsequently its brightness) is much lower thanthat of a single diode bar. There are, however, several techniques forsignificantly mitigating this problem, e.g., by spatial interleaving ofthe outputs of different diode stacks, by polarization coupling, or bywavelength multiplexing. Various types of high-power beam shapers andrelated devices have been developed for such purposes. Diode stacks mayprovide extremely high output powers (e.g. hundreds or thousands ofwatts).

In an aspect, embodiments of the invention feature a laser system thatincludes or consists essentially of an array of beam emitters eachemitting a beam having a fast diverging axis and a slow diverging axis,a fast-axis collimating lens for collimating the beams along the fastdiverging axis, a slow-axis collimating lens for reducing divergence ofthe beams along the slow diverging axis, an optical rotator for rotatingthe beams, focusing optics for focusing the rotated beams toward adispersive element, a dispersive element for receiving and dispersingthe focused beams, and a partially reflective output coupler forreceiving the dispersed beams, reflecting a first portion thereof backtoward the dispersive element, and transmitting a second portion thereofas a multi-wavelength output beam. Each of the emitted beams may have adifferent wavelength. The fast-axis collimating lens is disposedoptically downstream of the array of beam emitters. The slow-axiscollimating lens is disposed optically downstream of the fast-axiscollimating lens. The optical rotator is disposed optically downstreamof the slow-axis collimating lens. The focusing optics are disposedoptically downstream of the optical rotator. The dispersive element isdisposed optically downstream of the focusing optics. The partiallyreflective output coupler is disposed optically downstream of thedispersive element.

Embodiments of the invention may include one or more of the following inany of a variety of combinations. The dispersive element may include orconsist essentially of a diffraction grating. The focusing optics mayinclude or consist essentially of a cylindrical lens and/or acylindrical mirror. The optical rotator may include or consistessentially of two spaced-apart cylindrical lenses. The spacing betweenthe two spaced-apart cylindrical lenses may be less than approximately 2mm, or even less than approximately 1.8 mm. The spacing between the twospaced-apart cylindrical lenses may range between approximately 0.5 mmand approximately 2 mm, or may range between approximately 0.5 mm andapproximately 1.8 mm. The spacing between the two spaced-apartcylindrical lenses may be approximately 0.5 mm. An index of refractionof the optical rotator may be greater than approximately 1.5, or evengreater than approximately 1.7 or greater than approximately 1.8. Anindex of refraction of the optical rotator may range betweenapproximately 1.5 and approximately 2.3, or may range betweenapproximately 1.7 and approximately 2.3. An index of refraction of theoptical rotator may be approximately 2.3. The focal length of theoptical rotator may be less than approximately 2 mm, or even less thanapproximately 1.8 mm. The focal length of the optical rotator may rangebetween approximately 0.5 mm and approximately 2 mm, or may rangebetween approximately 0.5 mm and approximately 1.8 mm. The focal lengthof the optical rotator may be approximately 0.5 mm. The multi-wavelengthoutput beam may be coupled into an optical fiber.

In another aspect, embodiments of the invention feature a laserapparatus that includes or consists essentially of an array of beamemitters each emitting a beam of a different wavelength, each emittedbeam having a fast diverging axis and a slow diverging axis, a hybridlens having (i) a first surface for collimating the beams along the fastdiverging axis, and (ii) a second surface for reducing divergence of thebeams along the slow diverging axis, the first surface being disposedoptically downstream of the second surface, an optical rotator forrotating the beams, focusing optics for focusing the rotated beamstoward a dispersive element, a dispersive element for receiving anddispersing the focused beams, and a partially reflective output couplerfor receiving the dispersed beams, reflecting a first portion thereofback toward the dispersive element, and transmitting a second portionthereof as a multi-wavelength output beam. The hybrid lens is disposedoptically downstream of the array of beam emitters. The optical rotatoris disposed optically downstream of the hybrid lens. The focusing opticsare disposed optically downstream of the optical rotator. The dispersiveelement is disposed optically downstream of the focusing optics. Thepartially reflective output coupler is disposed optically downstream ofthe dispersive element.

Embodiments of the invention may include one or more of the following inany of a variety of combinations. The distance between the secondsurface of the hybrid lens and the array of beam emitters may result inincomplete collimation of the beams along the slow diverging axis. Thehybrid lens may include or consist essentially of a fast-axiscollimating lens optically bonded, at an interface, to one or moreslow-axis collimating lenses. At least one (i.e., even all) of theslow-axis collimating lenses may include or consist essentially of acylindrical Fresnel lens. The hybrid lens may include or consistessentially of a unitary optical component having shaped first andsecond surfaces. The second surface of the hybrid lens may be shaped asa plurality of lenses, e.g., cylindrical Fresnel lenses. The spacing ofthe lenses of the second surface of the hybrid lens may be substantiallyequal to a spacing of the array of beam emitters. The dispersive elementmay include or consist essentially of a diffraction grating. Thefocusing optics may include or consist essentially of a cylindrical lensand/or a cylindrical mirror. The optical rotator may include or consistessentially of two spaced-apart cylindrical lenses. The spacing betweenthe two spaced-apart cylindrical lenses may be less than approximately 2mm, or even less than approximately 1.8 mm. The spacing between the twospaced-apart cylindrical lenses may range between approximately 0.5 mmand approximately 2 mm, or may range between approximately 0.5 mm andapproximately 1.8 mm. The spacing between the two spaced-apartcylindrical lenses may be approximately 0.5 mm. An index of refractionof the optical rotator may be greater than approximately 1.5, or evengreater than approximately 1.7 or greater than approximately 1.8. Anindex of refraction of the optical rotator may range betweenapproximately 1.5 and approximately 2.3, or may range betweenapproximately 1.7 and approximately 2.3. An index of refraction of theoptical rotator may be approximately 2.3. The focal length of theoptical rotator may be less than approximately 2 mm, or even less thanapproximately 1.8 mm. The focal length of the optical rotator may rangebetween approximately 0.5 mm and approximately 2 mm, or may rangebetween approximately 0.5 mm and approximately 1.8 mm. The focal lengthof the optical rotator may be approximately 0.5 mm. The multi-wavelengthoutput beam may be coupled into an optical fiber.

These and other objects, along with advantages and features of thepresent invention herein disclosed, will become more apparent throughreference to the following description, the accompanying drawings, andthe claims. Furthermore, it is to be understood that the features of thevarious embodiments described herein are not mutually exclusive and mayexist in various combinations and permutations. As used herein, theterms “substantially” and “approximately” mean±10%, and in someembodiments, ±5%. The term “consists essentially of” means excludingother materials that contribute to function, unless otherwise definedherein. Nonetheless, such other materials may be present, collectivelyor individually, in trace amounts. Herein, the terms “radiation” and“light” are utilized interchangeably unless otherwise indicated.

BRIEF DESCRIPTION OF THE DRAWINGS

In the drawings, like reference characters generally refer to the sameparts throughout the different views. Also, the drawings are notnecessarily to scale, emphasis instead generally being placed uponillustrating the principles of the invention. In the followingdescription, various embodiments of the present invention are describedwith reference to the following drawings, in which:

FIG. 1A is a schematic of a wavelength beam combining (WBC) method alongthe array dimension of a single row of emitters in accordance withembodiments of the invention;

FIG. 1B is a schematic of a WBC method along the array dimension of atwo-dimensional array of emitters in accordance with embodiments of theinvention;

FIG. 1C is a schematic of a WBC method along the stack dimension of atwo-dimensional array of emitters in accordance with embodiments of theinvention;

FIG. 2 is a schematic showing the effects of smile in a WBC method alongthe stack dimension of a two-dimensional array of diode laser emittersin accordance with embodiments of the invention;

FIG. 3A is a schematic of a WBC system including an optical rotatorselectively rotating a one-dimensional array of beams in accordance withembodiments of the invention;

FIG. 3B is a schematic of a WBC system including an optical rotatorselectively rotating a two-dimensional array of beams in accordance withembodiments of the invention;

FIG. 3C is a schematic of a WBC system including an optical rotatorselectively reorienting a two-dimensional array of beams in accordancewith embodiments of the invention;

FIG. 3D illustrates output profile views of the system of FIG. 3C withand without an optical rotator in accordance with embodiments of theinvention;

FIGS. 4A-4C illustrate examples of optical rotators in accordance withembodiments of the invention;

FIGS. 5A-5C illustrate related methods for placing combining elements togenerate one-dimensional or two-dimensional laser elements;

FIG. 6 illustrates a WBC embodiment having a spatial repositioningelement in accordance with embodiments of the invention;

FIG. 7 illustrates an embodiment of a two-dimensional array of emittersbeing reconfigured before a WBC step and individual beam rotation afterthe WBC step in accordance with embodiments of the invention;

FIG. 8 illustrates the difference between slow and fast WBC inaccordance with embodiments of the invention;

FIG. 9A illustrates embodiments using an optical rotator before WBC inboth a single and stacked array configurations in accordance withembodiments of the invention;

FIG. 9B illustrates additional embodiments using an optical rotatorbefore WBC in accordance with embodiments of the invention;

FIG. 10 is illustrative of a single semiconductor chip emitter inaccordance with embodiments of the invention;

FIG. 11 is a schematic of a WBC system;

FIGS. 12 and 13 are schematics of WBC systems in accordance withembodiments of the invention;

FIG. 14 is a three-dimensional view of an exemplary hybrid lens inaccordance with embodiments of the invention; and

FIG. 15 is a three-dimensional view of a cylinder Fresnel lens, one ormore of which may be portions of a hybrid lens in accordance withembodiments of the invention.

DETAILED DESCRIPTION

Aspects and embodiments relate generally to the field of scaling lasersources to high-power and high-brightness using an external cavity and,more particularly, to methods and apparatus for external-cavity beamcombining using both one-dimensional or two-dimensional laser sources.In one embodiment the external cavity system includes one-dimensional ortwo-dimensional laser elements, an optical system, a dispersive element,and a partially reflecting element. An optical system is one or moreoptical elements that perform two basic functions. The first function isto overlap all the laser elements along the beam combining dimensiononto a dispersive element. The second function is to ensure all theelements along the non-beam combining dimension are propagating normalto the output coupler. In various embodiments, the optical systemintroduces as little loss as possible. As such, these two functions willenable a single resonance cavity for all the laser elements.

In another embodiment the WBC external cavity system includes wavelengthstabilized one-dimensional or two-dimensional laser elements, an opticalsystem, and a dispersive element. One-dimensional or two-dimensionalwavelength stabilized laser elements, with unique wavelength, can beaccomplished using various means such as laser elements with feedbackfrom wavelength chirped Volume Bragg grating, distributed feedback (DFB)laser elements, or distributed Bragg reflector (DBR) laser elements.Here the main function of the optical system is to overlap all the beamsonto a dispersive element. When there is no output coupler mirrorexternal to the wavelength-stabilized laser element, having parallelbeams along the non-beam-combining dimension is less important. Aspectsand embodiments further relate to high-power and/or high-brightnessmulti-wavelength external-cavity lasers that generate an overlapping orcoaxial beam from very low output power to hundreds and even tomegawatts of output power.

In particular, aspects and embodiments are directed to a method andapparatus for manipulating the beams emitted by the laser elements ofthese external-cavity systems and combining them using a WBC method toproduce a desired output profile. Wavelength beam combining methods havebeen developed to combine asymmetrical beam elements across theirrespective slow or fast axis dimension. One advantage of embodiments ofthe present invention is the ability to selectively-reconfigure inputbeams either spatially or by orientation to be used in slow and fastaxis WBC methods, as well as a hybrid of the two. Another advantage isthe ability to selectively-reconfigure input beams when there is afixed-position relationship to other input beams.

FIG. 1A illustrates a basic WBC architecture. In this particularillustration, WBC is performed along the array dimension or slowdimension for broad-area emitters. Individual beams 104 are illustratedin the figures by a dash or single line, where the length or longerdimension of the beam represents the array dimension or slow divergingdimension for broad-area emitters and the height or shorter dimensionrepresents the fast diverging dimension. (See also the left side of FIG.8). In this related art, a diode bar 102 having four emitters isillustrated. The emitters are aligned in a manner such that the slowdimension ends of each emitted beam 104 are aligned to one another sideby side along a single row—sometimes referred to as an array. However,it is contemplated that any lasing elements may be used and inparticular laser elements with broad gain bandwidth. Typically acollimation lens 106 is used to collimate each beam along the fastdiverging dimension. In some cases the collimation optics can becomposed of separate fast axis collimation lenses and slow axiscollimation lenses. Typically, transform optic 108 is used to combineeach beam along the WBC dimension 110 as shown by the input front view112. Transform optic 108 may be a cylindrical or spherical lens ormirror. The transform optic 108 then overlaps the combined beam onto adispersive element 114 (here shown as a reflecting diffraction grating).The first-order diffracted beams are incident onto a partiallyreflecting mirror. The laser resonator is formed between the back facetof the laser elements and the partially reflecting mirror. As such, thecombined beam is then transmitted as a single output profile onto anoutput coupler 116. This output coupler then transmits the combinedbeams 120, as shown by the output front view 118. It is contemplatedcreating a system devoid of an output coupler. For instance, aone-dimensional or two-dimensional system with wavelength stabilizedlaser elements and each having a unique wavelength may be accomplishedin a few ways. One system or method uses laser elements with feedbackfrom an external wavelength chirped Volume Bragg grating along the beamcombining dimension. Another uses internal distributed feedback (DFB)laser elements or internal distributed Bragg reflector (DBR) laserelements. In these systems, the single output profile transmitted fromthe dispersive element would have the same profile as 118. The outputcoupler 116 may be a partially reflective mirror or surface or opticalcoating and act as a common front facet for all the laser elements indiode array 102. A portion of the emitted beams is reflected back intothe optical gain and/or lasing portion of diode array 102 in thisexternal cavity system 100 a. An external cavity is a lasing systemwhere the secondary mirror is displaced at a distance away from theemission aperture or facet (not labeled) of each laser emitter.Generally, in an external cavity additional optical elements are placedbetween the emission aperture or facet and the output coupler orpartially reflective surface.

Similarly, FIG. 1B illustrates a stack of laser diode bars each havingfour emitters where those bars are stacked three high. Like FIG. 1A, theinput front view 112 of FIG. 1B, which in this embodiment is atwo-dimensional array of emitters, is combined to produce the outputfront view 118 or a single column of emitters 120. The emitted beams inexternal cavity 100 b were combined along the array dimension. Heretransform optic 108 is a cylindrical lens used to combine the beamsalong the array. However, a combination of optical elements or opticalsystem may be used as such that the optical elements arrange for all thebeams to overlap onto the dispersive element and ensure all the beamsalong the non-beam-combining dimension are propagating normal to theoutput coupler. A simple example of such an optical system would be asingle cylindrical lens with the appropriate focal length along thebeam-combining dimension and two cylindrical lenses that form an afocaltelescope along the non-beam-combining dimension wherein the opticalsystem projects images onto the partially reflecting mirrors. Manyvariations of this optical system can be designed to accomplish the samefunctions.

The array dimension FIG. 1B is also the same axis as the slow dimensionof each emitted beam in the case of multimode diode laser emitters.Thus, this WBC system may also be called slow axis combining, where thecombining dimension is the same dimension of the beams.

By contrast, FIG. 1C illustrates a stack 150 of laser diode arrays 102forming a two-dimensional array of emitters, as shown by 120, whereinstead of combining along the array dimension as in FIGS. 1A and 1B,the WBC dimension now follows along the stack dimension of the emitters.Here, the stacking dimension is also aligned with the fast axisdimension of each of the emitted beams. The input front view 112 is nowcombined to produce the output front view 118 wherein a single column120 of emitters is shown.

There are various drawbacks to all three configurations. One of the maindrawbacks of configuration shown in FIGS. 1A and 1B is that beamcombining is performed along the array dimension. As suchexternal-cavity operation is highly dependent on imperfections of thediode array. If broad-area semiconductor laser emitters are used thespectral utilization in the WBC system is not as efficient as if beamcombining is performed along the fast axis dimension. One of the maindrawbacks of configurations shown in FIG. 1C is that external beamshaping for beam symmetrization is required for efficient coupling intoa fiber. The beam symmetrization optics needed for a high power systemhaving a large number of emitters may be complex and non-trivial.Another disadvantage of configuration 1C is that the output beam qualityis limited to that of a single laser bar. Typical semiconductor or diodelaser bars have 19 to 49 emitters per bar with nearlydiffraction-limited beam quality in one dimension and beam quality thatis several hundreds of times diffraction-limited along the arraydimension. After beam symmetrization the output beam 120 can be coupledinto at best a 100 μm/0.22 Numerical Aperture (NA) fiber. To obtainhigher beam quality a small number of emitter bars is needed. Forexample to couple into 50 μm/0.22 NA fiber a five-emitter output beam isneeded. In many industrial laser applications a higher brightness laserbeam is required. For example, in some applications a two-emitter outputbeam is needed instead of 19 or 49. The two-emitter output beam can becoupled to a smaller core diameter fiber with much more engineeringtolerance and margin. This additional margin in core diameter and NA iscritical for reliable operation at high power (kW-class) power levels.While it is possible to procure five-emitter or two-emitter bars thecost and complexity is generally much higher as compare to a standard 19or 49 emitter bars because of the significantly reduced power per bar.In this disclosure, we disclose methods to remove all of the aboveshortcomings.

The previous illustrations, FIGS. 1A-1C, showed pre-arranged or fixedposition arrays and stacks of laser emitters. Generally, arrays orstacks are arranged mechanically or optically to produce a particularone-dimensional or two-dimensional profile. Thus, fixed-position is usedto describe a preset condition of laser elements where the laserelements are mechanically fixed with respect to each other as in thecase of semiconductor or diode laser bars having multiple emitters orfiber lasers mechanically spaced apart in V-grooves, as well as otherlaser emitters that come packaged with the emitters in a fixed position.

Alternatively, fixed position may refer to the secured placement of alaser emitter in a WBC system where the laser emitter is immobile.Pre-arranged refers to an optical array or profile that is used as theinput profile of a WBC system. Often times the pre-arranged position isa result of emitters configured in a mechanically fixed position.Pre-arranged and fixed position may also be used interchangeably.Examples of fixed-position or pre-arranged optical systems are shown inFIGS. 5A-C.

FIGS. 5A-5C refer to prior art illustrated examples of opticallyarranged one and two-dimensional arrays. FIG. 5A illustrates anoptically arranged stack of individual optical elements 510. Mirrors 520are used to arrange the optical beams from optical elements 530, eachoptical element 530 having a near field image 540, to produce an image550 (which includes optical beams from each optical element 530)corresponding to a stack 560 (in the horizontal dimension) of theindividual optical elements 510. Although the optical elements 500 maynot be arranged in a stack, the mirrors 520 arrange the optical beamssuch that the image 550 appears to correspond to the stack 560 ofoptical elements 510. Similarly, in FIG. 5B, the mirrors 520 can be usedto arrange optical beams from diode bars or arrays 570 to create animage 550 corresponding to a stack 560 of diode bars or arrays 575. Inthis example, each diode bar or array 570 has a near field image 540that includes optical beams 545 from each individual element in the baror array. Similarly, the minors 520 may also be used to opticallyarrange laser stacks 580 into an apparent larger overall stack 560 ofindividual stacks 585 corresponding to image 550, as shown in FIG. 5C.

Nomenclature, used in prior art to define the term “array dimension,”referred to one or more laser elements placed side by side where thearray dimension is also along the slow axis. One reason for thisnomenclature is diode bars with multiple emitters are often arranged inthis manner where each emitter is aligned side by side such that eachbeam's slow dimension is along a row or array. For purposes of thisapplication, an array or row refers to individual emitters or beamsarranged across a single dimension. The individual slow or fastdimension of the emitters of the array may also be aligned along thearray dimension, but this alignment is not to be assumed. This isimportant because some embodiments described herein individually rotatethe slow dimension of each beam aligned along an array or row.Additionally, the slow axis of a beam refers to the wider dimension ofthe beam and is typically also the slowest diverging dimension, whilethe fast axis refers to the narrower dimension of the beam and istypically the fastest diverging dimension. The slow axis may also referto single mode beams

Additionally, some prior art defines the term “stack or stackingdimension” referred to as two or more arrays stacked together, where thebeams' fast dimension is the same as the stacking dimension. Thesestacks were pre-arranged mechanically or optically. However, forpurposes of this application a stack refers to a column of beams orlaser elements and may or may not be along the fast dimension.Particularly, as discussed above, individual beams or elements may berotated within a stack or column.

In some embodiments it is useful to note that the array dimension andthe slow dimension of each emitted beam are initially oriented acrossthe same axis; however, those dimensions, as described in thisapplication, may become oriented at an offset angle with respect to eachother. In other embodiments, the array dimension and only a portion ofthe emitters arranged along the array or perfectly aligned the same axisat a certain position in a WBC system. For example, the array dimensionof a diode bar may have emitters arranged along the array dimension, butbecause of smile (often a deformation or bowing of the bar) individualemitters' slow emitting dimension is slightly skewed or offset from thearray dimension.

Laser sources based on common “commercial, off-the-shelf” or COTS highpower laser diode arrays and stacks are based on broad-areasemiconductor or diode laser elements. Typically, the beam quality ofthese elements is diffraction-limited along the fast axis and many timesdiffraction-limited along the slow axis of the laser elements. It is tobe appreciated that although the following discussion may referprimarily to single emitter laser diodes, diode laser bars and diodelaser stacks, embodiments of the invention are not limited tosemiconductor or laser diodes and may be used with many different typesof laser and amplifier emitters, including fiber lasers and amplifiers,individually packaged diode lasers, other types of semiconductor lasersincluding quantum cascade lasers (QCLs), tapered lasers, ridge waveguide(RWG) lasers, distributed feedback (DFB) lasers, distributed Braggreflector (DBR) lasers, grating coupled surface emitting laser, verticalcavity surface emitting laser (VCSEL), and other types of lasers andamplifiers.

All of the embodiments described herein can be applied to WBC of diodelaser single emitters, bars, and stacks, and arrays of such emitters. Inthose embodiments employing stacking of diode laser elements, mechanicalstacking or optical stacking approaches can be employed. In addition,where an HR coating is indicated at the facet of a diode laser element,the HR coating can be replaced by an AR coating, provided that externalcavity optical components, including but not limited to a collimatingoptic and bulk HR mirror are used in combination with the AR coating.This approach is used, for example, with WBC of diode amplifierelements. Slow axis is also defined as the worse beam quality directionof the laser emission. The slow axis typically corresponds to thedirection parallel to the semiconductor chip at the plane of theemission aperture of the diode laser element. Fast axis is defined asthe better beam quality direction of the laser emission. Fast axistypically corresponds to the direction perpendicular to thesemiconductor chip at the plane of the emission aperture of the diodelaser element.

An example of a single semiconductor chip emitter 1000 is shown in FIG.10. The aperture 1050 is also indicative of the initial beam profile.Here, the height 1010 at 1050 is measured along the stack dimension.Width 1020 at 1050 is measured along the array dimension. Height 1010 isthe shorter dimension at 1050 than width 1020. However, height 1010expands faster or diverges to beam profile 1052, which is placed at adistance away from the initial aperture 1050. Thus, the fast axis isalong the stack dimension. Width 1020 which expands or diverges at aslower rate as indicated by width 1040 being a smaller dimension thanheight 1030. Thus, the slow axis of the beam profile is along the arraydimension. Though not shown, multiple single emitters such as 1000 maybe arranged in a bar side by side along the array dimension.

Drawbacks for combining beams primarily along their slow axis dimensionmay include: reduced power and brightness due to lasing inefficienciescaused by pointing errors, smile and other misalignments. As illustratedin FIG. 2, a laser diode array with smile, one often caused by the diodearray being bowed in the middle sometimes caused by the diode laser barmounting process, is one where the individual emitters along the arrayform a typical curvature representative of that of a smile. Pointingerrors are individual emitters along the diode bar emitting beams at anangle other than normal from the emission point. Pointing error may berelated to smile, for example, the effect of variable pointing along thebar direction of a diode laser bar with smile when the bar is lensed bya horizontal fast axis collimating lens. These errors cause feedbackfrom the external cavity, which consists of the transform lens, grating,and output coupler, not to couple back to the diode laser elements. Somenegative effects of this miscoupling are that the WBC laser breakswavelength lock and the diode laser or related packaging may be damagedfrom miscoupled or misaligned feedback not re-entering the optical gainmedium. For instance the feedback may hit some epoxy or solder incontact or in close proximity to a diode bar and cause the diode bar tofail catastrophically.

Row 1 of FIG. 2 shows a single laser diode bar 202 without any errors.The embodiments illustrated are exemplary of a diode bar mounted on aheat sink and collimated by a fast-axis collimation optic 206. Column Ashows a perspective or 3-D view of the trajectory of the output beams211 going through the collimation optic 206. Column D shows a side viewof the trajectory of the emitted beams 211 passing through thecollimation optic 206. Column B shows the front view of the laser facetwith each individual laser element 213 with respect to the collimationoptic 206. As illustrated in row 1, the laser elements 213 are perfectlystraight. Additionally, the collimation optic 206 is centered withrespect to all the laser elements 213. Column C shows the expectedoutput beam from a system with this kind of input. Row 2 illustrates adiode laser array with pointing error. Shown by column B of row 2 thelaser elements and collimation optic are slightly offset from eachother. The result, as illustrated, is the emitted beams having anundesired trajectory that may result in reduced lasing efficiency for anexternal cavity. Additionally, the output profile may be offset torender the system ineffective or cause additional modifications. Row 3shows an array with packaging error. The laser elements no longer sit ona straight line, and there is curvature of the bar. This is sometimesreferred to as “smile.” As shown on row 3, smile may introduce even moretrajectory problems as there is no uniform path or direction common tothe system. Column D of row 3 further illustrates beams 211 exiting atvarious angles. Row 4 illustrates a collimation lens unaligned with thelaser elements in a twisted or angled manner. The result is probably theworst of all as the output beams generally have the most collimation ortwisting errors. In most systems, the actual error in diode arrays andstacks is a combination of the errors in rows 2, 3, and 4. In bothmethods 2 and 3, using VBG's and diffraction gratings, laser elementswith imperfections result in output beams no longer pointing parallel tothe optical axis. These off optical axis beams result in each of thelaser elements lasing at different wavelengths. The plurality ofdifferent wavelengths increases the output spectrum of the system tobecome broad as mentioned above.

One of the advantages of performing WBC along the stacking dimension(here also primarily the fast dimension) of a stack of diode laser barsis that it compensates for smile as shown in FIG. 2. Pointing and otheralignment errors are not compensated by performing WBC along the arraydimension (also primarily slow dimension). A diode bar array may have arange of emitters typically from 19 to 49 or more. As noted, diode bararrays are typically formed such that the array dimension is where eachemitter's slow dimension is aligned side by side with the otheremitters. As a result, when using WBC along the array dimension, whethera diode bar array has 19 or 49 emitters (or any other number ofemitters), the result is that of a single emitter. By contrast, whenperforming WBC along the orthogonal or fast dimension of the same singlediode bar array, the result is each emitted beam increases in spectralbrightness, or narrowed spectral bandwidth, but there is not a reductionin the number of beams (equivalently, there is not an increase inspatial brightness).

This point is illustrated in FIG. 8. On the left of FIG. 8 is shown afront view of an array of emitters 1 and 2 where WBC along the slowdimension is being performed. Along the right side using the same arrays1 and 2, WBC along the fast dimension is being performed. When comparingarray 1, WBC along the slow dimension reduces the output profile to thatof a single beam, while WBC along the fast dimension narrows thespectral bandwidth, as shown along the right side array 1, but does notreduce the output profile size to that of a single beam.

Using COTS diode bars and stacks the output beam from beam combiningalong the stack dimension is usually highly asymmetric. Symmetrization,or reducing the beam profile ratio closer to equaling one, of the beamprofile is important when trying to couple the resultant output beamprofile into an optical fiber. Many of the applications of combining aplurality of laser emitters require fiber coupling at some point in anexpanded system. Thus, having greater control over the output profile isanother advantage of the application.

Further analyzing array 2 in FIG. 8 shows the limitation of the numberof emitters per laser diode array that is practical for performing WBCalong the fast dimension if very high brightness symmetrization of theoutput profile is desired. As discussed above, typically the emitters ina laser diode bar are aligned side by side along their slow dimension.Each additional laser element in a diode bar is going to increase theasymmetry in the output beam profile. When performing WBC along the fastdimension, even if a number of laser diode bars are stacked on eachother, the resultant output profile will still be that of a single laserdiode bar. For example if one uses a COTS 19-emitter diode laser bar,the best that one can expect is to couple the output into a 100 μm/0.22NA fiber. Thus, to couple into a smaller core fiber lower number ofemitters per bar is required. One could simply fix the number ofemitters in the laser diode array to 5 emitters in order to help withthe symmetrization ratio; however, fewer emitters per laser diode bararray generally results in an increase of cost of per bar or cost perWatt of output power. For instance, the cost of diode bar having 5emitters may be around $2,000 whereas the cost of diode bar having 49emitters may be around roughly the same price. However, the 49 emitterbar may have a total power output of up to an order-of-magnitude greaterthan that of the 5 emitter bar. Thus, it would be advantageous for a WBCsystem to be able to achieve a very high brightness output beams usingCOTS diode bars and stacks with larger number of emitters. An additionaladvantage of bars with larger number of emitters is the ability tode-rate the power per emitter to achieve a certain power level per barfor a given fiber-coupled power level, thereby increasing the diodelaser bar lifetime or bar reliability.

One embodiment that addresses this issue is illustrated in FIG. 3A,which shows a schematic of WBC system 300 a with an optical rotator 305placed after collimation lenses 306 and before the transform optic 308.It should be noted the transform optic 308 may include or consistessentially of a number of lenses or mirrors or other opticalcomponents. The optical rotator 305 individually rotates the fast andslow dimension of each emitted beam shown in the input front view 312 toproduce the re-oriented front view 307. It should be noted that theoptical rotators can selectively rotate each beam individuallyirrespective of the other beams or can rotate all the beams through thesame angle simultaneously. It should also be noted that a cluster of twoor more beams can be rotated simultaneously. The resulting output afterWBC is performed along the array dimension is shown in output front view318 as a single emitter. Dispersive element 314 is shown as a reflectiondiffraction grating, but may also be a dispersive prism, a grism(prism+grating), transmission grating, and Echelle grating. Thisparticular embodiment illustrated shows only four laser emitters;however, as discussed above this system could take advantage of a laserdiode array that included many more elements, e.g., 49. This particularembodiment illustrated shows a single bar at a particular wavelengthband (example at 976 nm) but in actual practice it may be composed ofmultiple bars, all at the same particular wavelength band, arrangedside-by-side. Furthermore, multiple wavelength bands (example 976 nm,915 nm, and 808 nm), with each band composing of multiple bars, may becombined in a single cavity. Because WBC was performed across the fastdimension of each beam it easier to design a system with a higherbrightness (higher efficiency due to insensitivity due to barimperfections); additionally, narrower bandwidth and higher power outputare all achieved. As previously discussed it should be noted that someembodiments WBC system 300 a may not include output coupler 316 and/orcollimation lens(es) 306. Furthermore, pointing errors and smile errorsare compensated for by combining along the stack dimension (In thisembodiment this is also the fast dimension). FIG. 3B, shows animplementation similar to 3A except that a stack 350 of laser arrays 302forms a 2-D input profile 312. Cavity 300 b similarly consists ofcollimation lens(es) 306, optical rotator 305, transform optic 308,dispersive element 308 (here a diffraction grating), and an outputcoupler 316 with a partially reflecting surface. Each of the beams isindividually rotated by optical rotator 305 to form an after rotatorprofile 307. The WBC dimension is along the array dimension, but withthe rotation each of the beams will be combined across their fast axis.Fast axis WBC produces outputs with very narrow line widths and highspectral brightness. These are usually ideal for industrial applicationssuch as welding. After transform optic 308 overlaps the rotated beamsonto dispersive element 314 a single output profile is produced andpartially reflected back through the cavity into the laser elements. Theoutput profile 318 is now comprised of a line of three (3) beams that isquite asymmetric.

FIG. 3C shows the same implementation when applied to 2-D laserelements. The system consists of 2-D laser elements 302, optical rotator305, transform optical system (308 and 309 a-b) a dispersive element314, and a partially reflecting mirror 316. FIG. 3C illustrates a stack350 of laser diode bars 302 with each bar having an optical rotator 305.Each of the diode bars 302 (three total) as shown in external cavity 300c includes four emitters. After input front view 312 is reoriented byoptical rotator 305, reoriented front view 307 now the slow dimension ofeach beam aligned along the stack dimension. WBC is performed along thedimension, which is now the slow axis of each beam and the output frontview 318 now comprises single column of beams with each beam's slowdimension oriented along the stack dimension. Optic 309 a and 309 bprovide a cylindrical telescope to image along the array dimension. Thefunction of the three cylindrical lenses is two-fold. The middlecylindrical lens is the transform lens and its main function is tooverlap all the beams onto the dispersive element. The two othercylindrical lenses 309 a and 309 b form an afocal cylindrical telescopealong the non-beam combining dimension. Its main function is to makesure all laser elements along the non-beam combining are propagationnormal to the partially reflecting mirror. As such the implementation asshown in FIG. 3C has the same advantages as the one shown in FIG. 1C.However, unlike the implementation as shown in FIG. 1C the output beamis not the same as the input beam. The number of emitters in the outputbeam 318 in FIG. 3C is the same as the number of bars in the stack. Forexample, if the 2-D laser source consists of a three-bar stack with eachbar composed of 49 emitters, then the output beam in FIG. 1C is a singlebar with 49 emitters. However, in FIG. 3C the output beam is a singlebar with only three emitters. Thus, the output beam quality orbrightness is more than one order of magnitude higher. This brightnessimprovement is very significant for fiber-coupling. For higher power andbrightness scaling multiple stacks can be arranged side-by-side.

To illustrate this configuration further, for example, assume WBC is tobe performed of a three-bar stack, with each bar comprising of 19emitters. So far, there are three options. First, wavelength beamcombining can be performed along the array dimension to generate threebeams as shown in FIG. 1B. Second, wavelength beam combining can beperformed along the stack dimension to generate 19 beams a shown FIG.1C. Third, wavelength beam combining can be performed along the arraydimension using beam rotator to generate 19 beams as shown FIG. 3C.There are various trade-offs for all three configuration. The first casegives the highest spatial brightness but the lowest spectral brightness.The second case gives the lowest spatial brightness with moderatespectral brightness and beam symmetrization is not required to coupleinto a fiber. The third case gives the lowest spatial brightness but thehighest spectral brightness and beam symmetrization is required tocouple into an optical fiber. In some applications this more desirable.

To illustrate the reduction in asymmetry FIG. 3D has been drawn showingthe final output profile 319 a where the system of 300 b did not have anoptical rotator and output profile 319 b where the system includes anoptical rotator. Though these figures are not drawn to scale, theyillustrate an advantage achieved by utilizing an optical rotator, in asystem with this configuration where WBC is performed across the slowdimension of each beam. The shorter and wider 319 b is more suitable forfiber coupling than the taller and slimmer 319 a.

Examples of various optical rotators are shown in FIG. 4A-4C. FIG. 4Aillustrates an array of cylindrical lenses (419 a and 419 b) that causeinput beam 411 a to be rotated to a new orientation at 411 b. FIG. 4Bsimilarly shows input 411 a coming into the prism at an angle, whichresults in a new orientation or rotation beam 411 b. FIG. 4C illustratesan embodiment using a set of step mirrors 417 to cause input 411 a torotate at an 80-90 degree angle with the other input beams resulting ina new alignment of the beams 411 b where they are side by side alongtheir respective fast axis. These devices and others may cause rotationthrough both non-polarization sensitive as well as polarizationsensitive means. Many of these devices become more effective if theincoming beams are collimated in at least the fast dimension. It is alsounderstand that the optical rotators can selectively rotate the beams atvarious including less than 90 degrees, 90 degrees and greater than 90degrees.

The optical rotators in the previous embodiments may selectively rotateindividual, rows or columns, and groups of beams. In some embodiments aset angle of rotation, such as a range of 80-90 degrees is applied tothe entire profile or subset of the profile. In other instances, varyingangles of rotation are applied uniquely to each beam, row, column orsubset of the profile (see FIGS. 9A-B). For instance, one beam may berotated by 45 degrees in a clockwise direction while an adjacent beam isrotated 45 degrees in a counterclockwise direction. It is alsocontemplated one beam is rotated 10 degrees and another is rotated 70degrees. The flexibility the system provides may be applied to a varietyof input profiles, which in turn helps determine how the output profileis to be formed.

Performing WBC along an intermediate angle between the slow and fastdimension of the emitted beams is also well within the scope of theinvention (See for example 6 on FIG. 9B). Some laser elements asdescribed herein, produce electromagnetic radiation and include anoptical gain medium. When the radiation or beams exit the optical gainportion they generally are collimated along the slow and/or fastdimension through a series of micro lenses. From this point, theembodiments already described in this section included an opticalrotator that selectively and rotated each beam prior to the beams beingoverlapped by a transform lens along either the slow or the fastdimension of each beam onto a dispersive element. The output coupler mayor may not be coated to partially reflect the beams back into the systemto the laser element where the returned beams assist in generating moreexternal cavity feedback in the optical gain element portion until theyare reflected off a fully reflective mirror in the back portion of thelaser element. The location of the optical elements listed above andothers not listed are with respect to the second partially reflectivesurface helps decide whether the optical elements are within an externalcavity system or outside of the lasing cavity. In some embodiments, notshown, the second partially reflective mirror resides at the end of theoptical gain elements and prior to the collimating or rotating optics.

Another method for manipulating beams and configurations to takeadvantage of the various WBC methods includes using a spatialrepositioning element. This spatial repositioning element may be placedin an external cavity at a similar location as to that of an opticalrotator. For example, FIG. 6 shows a spatial repositioning element 603placed in the external cavity WBC system 600 after the collimatinglenses 606 and before the transform optic(s) 608. The purpose of aspatial repositioning element is to reconfigure an array of elementsinto a new configuration. FIG. 6 shows a three-bar stack with N elementsreconfigured to a six-bar stack with N/2 elements. Spatial repositioningis particularly useful in embodiments such as 600, where stack 650 is amechanical stack or one where diode bar arrays 602 and their outputbeams were placed on top of each other either mechanically or optically.With this kind of configuration the laser elements have a fixed-positionto one another. Using a spatial repositioning element can form a newconfiguration that is more ideal for WBC along the fast dimension. Thenew configuration makes the output profile more suitable for fibercoupling.

For example, FIG. 7 illustrates an embodiment wherein a two-dimensionalarray of emitters 712 is reconfigured during a spatial repositioningstep 703 by a spatial repositioning optical element such as an array ofperiscope mirrors. The reconfigured array shown by reconfigured frontview 707 is now ready for a WBC step 710 to be performed across the WBCdimension, which here is the fast dimension of each element. Theoriginal two-dimensional profile in this example embodiment 700 is anarray of 12 emitters tall and 5 emitters wide. After the array istransmitted or reflected by the spatial repositioning element a newarray of 4 elements tall and 15 elements wide is produced. In botharrays the emitters are arranged such that the slow dimension of each isvertical while the fast dimension is horizontal. WBC is performed alongthe fast dimension which collapses the 15 columns of emitters in thesecond array into 1 column that is 4 emitters tall. This output isalready more symmetrical than if WBC had been performed on the originalarray, which would have resulted in a single column 15 emitters tall. Asshown, this new output may be further symmetrized by an individuallyrotating step 705 rotating each emitter by 90 degrees. In turn, apost-WBC front view 721 is produced being the width of a single beamalong the slow dimension and stacked 4 elements high, which is a moresuitable for coupling into a fiber.

One way of reconfiguring the elements in a one-dimensional ortwo-dimensional profile is to make ‘cuts’ or break the profile intosections and realign each section accordingly. For example, in FIG. 7two cuts 715 were made in 713. Each section was placed side by side toform 707. These optical cuts can be appreciated if we note the elementsof 713 had a pre-arranged or fixed-position relationship. It is alsowell within the scope to imagine any number of cuts being made toreposition the initial input beam profile. Each of these sections may inaddition to being placed side by side, but on top and even randomized ifso desired.

Spatial repositioning elements may be comprised of a variety of opticalelements including periscope optics that are both polarized andnon-polarized as well as other repositioning optics. Step mirrors asshown in FIG. 4a may also be reconfigured to become a spatialrepositioning element.

Additional embodiments of the invention are illustrated in FIGS. 9A-9B.The system shown in 1 of FIG. 9A shows a single array of four beamsaligned side to side along the slow dimension. An optical rotatorindividually rotates each beam. The beams are then combined along thefast dimension and are reduced to a single beam by WBC. In thisarrangement it is important to note that the 4 beams could easily be 49or more beams. It may also be noted that if some of the emitters arephysically detached from the other emitters, the individual emitter maybe mechanically rotated to be configured in an ideal profile. Amechanical rotator may be comprised of a variety of elements includingfriction sliders, locking bearings, tubes, and other mechanismsconfigured to rotate the laser element. Once a desired position isachieved the laser elements may then be fixed into place. It is alsoconceived that an automated rotating system that can adjust the beamprofile depending on the desired profile may be implemented. Thisautomated system may either mechanically reposition a laser or opticalelement or a new optical element may be inserted in and out of thesystem to change the output profile as desired.

System 2 shown in FIG. 9A, shows a two-dimensional array having threestacked arrays with four beams each aligned along the slow dimension.(Similar to FIG. 3C) As this stacked array passes through an opticalrotator and WBC along the fast dimension a single column of three beamstall aligned top to bottom along the slow dimension is created. Again itis appreciated that if the three stacked arrays shown in this system had50 elements, the same output profile would be created, albeit one thatis brighter and has a higher output power.

System 3 in FIG. 9B, shows a diamond pattern of four beams wherein thebeams are all substantially parallel to one another. This pattern mayalso be indicative of a random pattern. The beams are rotated andcombined along the fast dimension, which results in a column of threebeams aligned along the slow dimension from top to bottom. Missingelements of diode laser bars and stacks due to emitter failure or otherreasons, is an example of System 3. System 4, illustrates a system wherethe beams are not aligned, but that one beam is rotated to be alignedwith a second beam such that both beams are combined along the fastdimension forming a single beam. System 4, demonstrates a number ofpossibilities that expands WBC methods beyond using laser diode arrays.For instance, the input beams in System 4 may be from carbon dioxide(CO₂) lasers, semiconductor or diode lasers, diode pumped fiber lasers,lamp-pumped or diode-pumped Nd:YAG lasers, Disk Lasers, and so forth.The ability to mix and match the type of lasers and wavelengths oflasers to be combined is another advantage of embodiments of the presentinvention.

System 5, illustrates a system where the beams are not rotated to befully aligned with WBC dimension. The result is a hybrid output thatmaintains many of the advantages of WBC along the fast dimension. Inseveral embodiments the beams are rotated a full 90 degrees to becomealigned with WBC dimension, which has often been the same direction ordimension as the fast dimension. However, System 5 and again System 6show that optical rotation of the beams as a whole (System 6) orindividually (System 5) may be such that the fast dimension of one ormore beams is at an angle theta or offset by a number of degrees withrespect to the WBC dimension. A full 90 degree offset would align theWBC dimension with the slow dimension while a 45 degree offset wouldorient the WBC dimension at an angle halfway between the slow and fastdimension of a beam as these dimension are orthogonal to each other. Inone embodiment, the WBC dimension has an angle theta at approximately 3degrees off the fast dimension of a beam.

FIG. 11 depicts an exemplary WBC system 1100 featuring a one-dimensionalor two-dimensional array of beam emitters 102 and a FAC lens 1110 forcollimating the beams from beam emitters 102 along the FA. The WBCsystem 1100 also includes an optical rotator 305 that rotates theindividual beams as detailed herein. The optical rotator 305 may includeor consist essentially of two cylindrical lenses 1120, 1130 separated bya distance 1140. Distance 1140 may be, for example, approximately equalto the sum of the focal lengths of lenses 1120, 1130. The WBC system1100 also includes focusing optics 108 (e.g., one or more cylindricallenses and/or mirrors, and/or one or more spherical lenses and/ormirrors) that combine the beams emitted by the emitters 102 to form acombined beam that propagates toward a dispersive element 114. Thedispersive element 114 (e.g., a diffraction grating, a dispersive prism,a grism (prism/grating), a transmission grating, or an Echelle grating)may be disposed approximately at the focal length of the focusing optics108. As described herein, the dispersive element 114 receives thecombined beam and transmits the beam as a multi-wavelength beam having ahigh brightness. The multi-wavelength beam is transmitted to a partiallyreflective output coupler 116 that transmits a portion of themulti-wavelength beam (e.g., to an optical fiber 1150) and reflects asecond portion of the multi-wavelength beam back toward the dispersiveelement 114 and thence to the emitters 102, forming an external lasingcavity. As mentioned above, the beam(s) traversing the optical rotator305 may continue to diverge, which may result in negative cross-talkbetween the FA and SA in the combined output beam.

As shown in FIG. 12, in order to minimize or reduce such cross-talkbetween the FA and SA, a WBC system 1200 features a SAC lens 1210optically downstream from the FAC lens 1110 and upstream of the opticalrotator 305. In various embodiments, the SAC lens 1210 collimates thebeams along the SA, but the SAC lens 1210 having a short focal lengthand being disposed so close to the beam emitters 102 results inincomplete collimation of the beams along the SA. The SAC lens 1210 mayinclude or consist essentially of a single lens or a one-dimensional ortwo-dimensional array of lenses (e.g., unified in a single opticalelement) that may each correspond to one of the beams from array 102.(FIG. 12 depicts beams 1220 propagating through the optical rotator 305in solid lines and as incompletely collimated compared to theoreticallyfully collimated beams 1230 shown in dashed lines; these may both becompared to theoretically uncollimated (as in FIG. 11) beams 1240 shownin dotted lines.) However, even this incomplete collimation helps toreduce negative cross-talk between the slow axis and the fast axis thatmay result when beams pass through the optical rotator 305. Suchcross-talk between the slow axis and the fast axis may deleteriouslyimpact (e.g., skew) the resulting combined beam and render opticalcoupling the combined beam (e.g., into optical fiber 1150) moredifficult. However, this may be addressed, at least in part, in variousembodiments of the invention via reducing the focal length of (and thusa separation 150 between) the lenses 1120, 1130 of the optical rotator305 (e.g., two cylindrical lenses).

The reduction in focal length and separation depends on the index ofmaterial. For example, the separation of optical rotators using fusedsilica that are available commercially may be a few millimeters inmagnitude. The typical output beam rotation in the far field may be onthe order of 20-40 degrees. By using a higher index glass the separationbetween the two lenses may be 2-3 times shorter. This reduction inseparation may result in the output beam rotation in the far field of afew degrees. This focal-length reduction may help minimize cross-talkbetween the slow axis and fast axis within the optical rotator 305 andimprove the profile of the combined output beam. In various embodiments,the optical rotator 305 and/or the lenses 1120, 1130 have a refractiveindex larger than 1.5, or even larger than approximately 1.7. In variousembodiments, the optical rotator 305 and/or the lenses 1120, 1130 have arefractive index ranging from 1.5 to approximately 2.3, or even toapproximately 2.5. In various embodiments, the optical rotator 305and/or the lenses 1120, 1130 have a refractive index ranging from 1.7 toapproximately 2.3. In various embodiments, the focal length of (and/orseparation 150 between) the lenses 1120, 1130 of the optical rotator 305is less than approximately 2 mm, or even less than approximately 1.8 mm.In various embodiments, the focal length of (and/or separation 150between) the lenses 1120, 1130 of the optical rotator 305 ranges betweenapproximately 0.5 mm and approximately 2 mm. In various embodiments, thefocal length of (and/or separation 150 between) the lenses 1120, 1130 ofthe optical rotator 305 ranges between approximately 0.5 mm andapproximately 1.8 mm.

Although FAC lens 1110 and SAC lens 1210 are depicted in FIG. 12 asbeing spatially separated by a small gap, in various embodiments of theinvention this gap may be absent, and/or the SAC lens may be opticallyupstream of the FAC lens. For example, the FAC lens 1110 and the SAClens 1210 may be replaced by a hybrid lens 1310 having a SAC-lensportion 1320 and a FAC-lens portion 1330, as shown in FIG. 13. As shown,the lens portions 1320, 1330 may be attached (e.g., optically bondedvia, for example, an optical adhesive) together at an interface 1340. Invarious embodiments, the hybrid lens 1310 lacks a discrete interface1340 and the lens portions 1320, 1330 are shaped together as a unifiedcomponent by, e.g., molding. FIG. 14 depicts an exemplary hybrid lens1400 in accordance with various embodiments of the present invention. Asshown, the hybrid lens 1400 includes or consists essentially of a FAClens 1410 on a first surface that faces away from the beam array 102 andan array of SAC lenses 1420 on a second surface that faces the beamarray 102. Each SAC lens 1420 may correspond to, and be substantiallyaligned with, a beam from the array 102. In various embodiments, eachlens in the array of SAC lenses 1420 may include or consist essentiallyof a cylindrical Fresnel lens 1500, and example of which is shown inFIG. 15. The lenses 1500 may be spaced along hybrid lens 1310 with apitch (or spacing) substantially equal to that of the individual beamemitters in the beam array 102.

The terms and expressions employed herein are used as terms ofdescription and not of limitation, and there is no intention, in the useof such terms and expressions, of excluding any equivalents of thefeatures shown and described or portions thereof, but it is recognizedthat various modifications are possible within the scope of theinvention claimed.

What is claimed is:
 1. A laser apparatus comprising: an array of beamemitters each emitting a beam of a different wavelength, each emittedbeam having a fast diverging axis and a slow diverging axis; a hybridlens disposed optically downstream of the array of beam emitters, thehybrid lens having (i) a first surface for collimating the beams alongthe fast diverging axis, and (ii) a second surface for reducingdivergence of the beams along the slow diverging axis; disposedoptically downstream of the hybrid lens, an optical rotator for rotatingthe beams; disposed optically downstream of the optical rotator,focusing optics for focusing the rotated beams toward a dispersiveelement; disposed optically downstream of the focusing optics, thedispersive element for receiving and dispersing the focused beams; anddisposed optically downstream of the dispersive element, a partiallyreflective output coupler for receiving the dispersed beams, reflectinga first portion thereof back toward the dispersive element, andtransmitting a second portion thereof as a multi-wavelength output beam.2. The laser apparatus of claim 1, wherein a distance between the hybridlens and the array of beam emitters is selected to incompletelycollimate the beams along the slow diverging axis and thereby introducecross-talk between the fast diverging axis and slow diverging axis ofeach of the beams.
 3. The laser apparatus of claim 1, wherein the hybridlens comprises a fast-axis collimating lens optically bonded, at aninterface, to one or more slow-axis collimating lenses.
 4. The laserapparatus of claim 3, wherein at least one of the slow-axis collimatinglenses comprises a cylindrical Fresnel lens.
 5. The laser apparatus ofclaim 1, wherein the hybrid lens comprises a fast-axis collimating lensoptically bonded, at an interface, to a plurality of slow-axiscollimating lenses.
 6. The laser apparatus of claim 5, wherein at leastone of the slow-axis collimating lenses comprises a cylindrical Fresnellens.
 7. The laser apparatus of claim 1, wherein the hybrid lensconsists essentially of a unitary optical component having shaped firstand second surfaces.
 8. The laser apparatus of claim 1, wherein thesecond surface of the hybrid lens is shaped as a plurality ofcylindrical Fresnel lenses.
 9. The laser apparatus of claim 8, wherein aspacing of the cylindrical Fresnel lenses is substantially equal to aspacing of the array of beam emitters.
 10. The laser apparatus of claim1, wherein the dispersive element comprises a diffraction grating. 11.The laser apparatus of claim 1, wherein the focusing optics comprises atleast one of a cylindrical lens or a cylindrical mirror.
 12. The laserapparatus of claim 1, wherein the optical rotator comprises twospaced-apart cylindrical lenses.
 13. The laser apparatus of claim 12,wherein a spacing between the two spaced-apart cylindrical lenses isless than approximately 2 mm.
 14. The laser apparatus of claim 1,wherein an index of refraction of the optical rotator is greater thanapproximately 1.5.
 15. The laser apparatus of claim 1, wherein a focallength of the optical rotator is less than approximately 2 mm.
 16. Thelaser apparatus of claim 1, further comprising an optical fiber intowhich the multi-wavelength output beam is coupled.
 17. The laserapparatus of claim 1, wherein the array of beam emitters comprises adiode bar, each of the beam emitters comprising a diode emitter withinthe diode bar.
 18. The laser apparatus of claim 1, wherein the firstsurface is disposed optically downstream of the second surface.
 19. Thelaser apparatus of claim 1, wherein the second surface is disposedoptically downstream of the first surface.